In this report we compare in detail high-\(p_{\rm T}\)  dijet and \(\rm {Z} +\) jet production by applying the Parton Branching (PB) formulation of TMD evolution [1]}, [2]} together with NLO calculations of the hard scattering process in the MadGraph5_aMC@NLO [3]} framework. In Ref. [4]} these PB TMD PDFs were applied to multijet production at large transverse momenta. We apply the same method to the calculation of \(\rm {Z} +\) jet production.
We propose to use the same kinematic region for the high-\(p_{\rm T}\)  dijet and \(\rm {Z} +\) jet production to allow a direct comparison of the measurements. At large enough \(p_{\rm T}\)  the mass of the Z-boson becomes negligible, and the different color and spin structure of the final states might allow to observe factorization - breaking effects by comparing the measurements to calculations assuming that factorization holds.
